Solving 2-Part Homework: Tips & Strategies

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Homework Statement


upload_2014-9-28_15-30-55.png


2. Homework Equations [/B]
See question

The Attempt at a Solution



Ok 1a) is dead simple. But I am struggeling with part b. I plug in all the variables. But cannot seem to get a and b... I do this:

(-b)(S_x)(a,b) = E(a,b) and then get

-b^2h/2= Ea and ah/2=E

I don't know.. Can you guys help me.
 

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Note that the b in the Hamiltonian is not the same b as that in the wave function ...
 
Well that is a big help thanks. haha. Although I am sure still not sure how to proceed to find the Energy states. Because when I multiply the X matrix with the S_x matrix I get the transpose of X...
 
Well, it is not really a transpose - you simply switch the elements (a transpose would take a column matrix to a row one). The energy states are simply the states for which ##H\chi = E\chi##, where ##E## is a number, i.e., the eigenstates of the Hamiltonian.
 
Ya I understand that. But how can I get back the orginal X to find E. Since, as you say the elements switch places of X.
 
So, what did you obtain for the eigenstates? If you have found the energy eigenstates, all you need to do is to check what the constant multiplying ##\chi## is after you apply the Hamiltonian to it.
 
\frac{-b\hbar}{2}\begin{pmatrix}<br /> 0&amp;1\\<br /> 1&amp;0\\<br /> \end{pmatrix}<br /> \begin{pmatrix}<br /> a\\<br /> b\\<br /> \end{pmatrix}=<br /> \frac{-b\hbar}{2}<br /> \begin{pmatrix}<br /> b\\<br /> a\\<br /> \end{pmatrix}<br />

Now what?
 
Well, to start I would call the ##b## in the ##\chi## ##c## instead to separate it from the ##b## in the Hamiltonian (or rename the Hamiltonian ##b## to ##B## ...). Now you need to solve the eigenvalue equation that states that this should be equal to ##E \chi##.
 
Which is preciously where I'm stuck. I get a relationship for a and b but don't know how to solve for them.
 
  • #10
I suggest starting by solving for the energy eigenvalue E.
 
  • #11
Then I just get what I had over X... Now sure how that helps. E should be a value and not contain matrices . How can I eliminate them?
 
  • #12
For the matrix equation to hold, it must hold for every element.
 
  • #13
\frac{-B\hbar}{2}\begin{pmatrix}<br /> 0&amp;1\\<br /> 1&amp;0\\<br /> \end{pmatrix}<br /> \begin{pmatrix}<br /> a\\<br /> b\\<br /> \end{pmatrix}=<br /> \frac{-B\hbar}{2}<br /> \begin{pmatrix}<br /> b\\<br /> a\\<br /> \end{pmatrix}=E<br /> \begin{pmatrix}<br /> a\\<br /> b\\<br /> \end{pmatrix}<br />
So that implies:

\frac{-B\hbar a}{2b} = E and \frac{-B\hbar b}{2a} = E

Equating the:

\frac{-B\hbar b}{2a} = \frac{-B\hbar a}{2b}

so
a^2=b^2

Which implies:

a=\pm b

But we have the relationship:

|a|^2+|b|^2=1

So plugging it in I get:

a=\frac{1}{\sqrt{2}} b=\pm \frac{1}{\sqrt{2}}

So how does this give me the ground state and the excited states? or the value for E.

Like I said I am not sure how to solve this problem. Please some more guidance.
 
  • #14
You are essentially done. You have two expressions for E in terms of a and b that you now know - so just insert them. The ##\pm## gives you two possible values of E - the lower one corresponding to the ground state and the other the excited.
 
  • #15
so the ground state is:

\frac{-B\hbar}{2} = E

and the excited state is:

\frac{B\hbar}{2} = E
 
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